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Keywords = electromagnetic duality symmetry

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32 pages, 438 KiB  
Article
Off-Shell Duality Invariance of Schwarzschild Perturbation Theory
by Adam R. Solomon
Particles 2023, 6(4), 943-974; https://doi.org/10.3390/particles6040061 - 7 Nov 2023
Cited by 3 | Viewed by 1365
Abstract
We explore the duality invariance of the Maxwell and linearized Einstein–Hilbert actions on a non-rotating black hole background. On-shell, these symmetries are electric–magnetic duality and Chandrasekhar duality, respectively. Off-shell, they lead to conserved quantities; we demonstrate that one of the consequences of these [...] Read more.
We explore the duality invariance of the Maxwell and linearized Einstein–Hilbert actions on a non-rotating black hole background. On-shell, these symmetries are electric–magnetic duality and Chandrasekhar duality, respectively. Off-shell, they lead to conserved quantities; we demonstrate that one of the consequences of these conservation laws is that even- and odd-parity metric perturbations have equal Love numbers. Along the way, we derive an action principle for the Fackerell–Ipser equation and Teukolsky–Starobinsky identities in electromagnetism. Full article
20 pages, 960 KiB  
Review
Symmetry and Quantum Features in Optical Vortices
by David L. Andrews
Symmetry 2021, 13(8), 1368; https://doi.org/10.3390/sym13081368 - 28 Jul 2021
Cited by 23 | Viewed by 3641
Abstract
Optical vortices are beams of laser light with screw symmetry in their wavefront. With a corresponding azimuthal dependence in optical phase, they convey orbital angular momentum, and their methods of production and applications have become one of the most rapidly accelerating areas in [...] Read more.
Optical vortices are beams of laser light with screw symmetry in their wavefront. With a corresponding azimuthal dependence in optical phase, they convey orbital angular momentum, and their methods of production and applications have become one of the most rapidly accelerating areas in optical physics and technology. It has been established that the quantum nature of electromagnetic radiation extends to properties conveyed by each individual photon in such beams. It is therefore of interest to identify and characterize the symmetry aspects of the quantized fields of vortex radiation that relate to the beam and become manifest in its interactions with matter. Chirality is a prominent example of one such aspect; many other facets also invite attention. Fundamental CPT symmetry is satisfied throughout the field of optics, and it plays significantly into manifestations of chirality where spatial parity is broken; duality symmetry between electric and magnetic fields is also involved in the detailed representation. From more specific considerations of spatial inversion, amongst which it emerges that the topological charge has the character of a pseudoscalar, other elements of spatial symmetry, beyond simple parity inversion, prove to repay additional scrutiny. A photon-based perspective on these features enables regard to be given to the salient quantum operators, paying heed to quantum uncertainty limits of observables. The analysis supports a persistence in features of significance for the material interactions of vortex beams, which may indicate further scope for suitably tailored experimental design. Full article
(This article belongs to the Section Physics)
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Figure 1

Figure 1
<p>(<b>a</b>) Phasor structure of an <math display="inline"><semantics> <mi>ℓ</mi> </semantics></math> = 1, <span class="html-italic">p</span> = 0 LG beam, cycling as it propagates; hue denotes the phase, colour intensity the level of irradiance; the latter vanishes along the propagation axis (green arrow) at the phase singularity. The orientation of the local wave-vector (normal to the wavefront surface) is azimuth-dependent, as indicated at positions of opposite phase by red and blue arrows. (<b>b</b>) <math display="inline"><semantics> <mi>ℓ</mi> </semantics></math> = 3, <span class="html-italic">p</span> = 0 LG beam, showing the mutually orthogonal disposition of the cylindrical components of a local wave-vector.</p>
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<p>(<b>a</b>) Colour-continuum representation of the phasor Φ for a vortex at <span class="html-italic">z</span> = 0: (<b>a</b>) topological charge <math display="inline"><semantics> <mi>ℓ</mi> </semantics></math> = 1, where phase <span class="html-italic">θ</span> = <span class="html-italic">ϕ</span>; (<b>b</b>) <math display="inline"><semantics> <mi>ℓ</mi> </semantics></math> = 2, phase <span class="html-italic">θ</span> = 2<span class="html-italic">ϕ</span> (<span class="html-italic">ϕ</span> = 0 as usual designating the notional <span class="html-italic">x</span>-axis). The phase gradient field, indicated by yellow arrows (twice the magnitude in the latter case), is constant in <span class="html-italic">θ</span>. Any shift <span class="html-italic">ϕ</span> →<span class="html-italic">ϕ</span> + <span class="html-italic">π</span> imparts a change of sign to the phasor in (<b>a</b>), as for all cases of odd <math display="inline"><semantics> <mi>ℓ</mi> </semantics></math>; the same shift in (<b>b</b>) retains the sign, as is true for all even values of <math display="inline"><semantics> <mi>ℓ</mi> </semantics></math>. The vector field <math display="inline"><semantics> <mstyle mathvariant="bold" mathsize="normal"> <msup> <mi>Φ</mi> <mo>′</mo> </msup> </mstyle> </semantics></math> of the phasor gradient varies non-uniformly in direction, its real and imaginary parts (respectively represented by blue and red arrows) having signs either parallel or antiparallel to the phase gradient, according to the quadrant in (<b>a</b>), and the octant in (<b>b</b>).</p>
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13 pages, 365 KiB  
Article
A Non-Local Action for Electrodynamics: Duality Symmetry and the Aharonov-Bohm Effect, Revisited
by Joan Bernabeu and Jose Navarro-Salas
Symmetry 2019, 11(10), 1191; https://doi.org/10.3390/sym11101191 - 21 Sep 2019
Cited by 9 | Viewed by 3679
Abstract
A non-local action functional for electrodynamics depending on the electric and magnetic fields, instead of potentials, has been proposed in the literature. In this work we elaborate and improve this proposal. We also use this formalism to confront the electric-magnetic duality symmetry of [...] Read more.
A non-local action functional for electrodynamics depending on the electric and magnetic fields, instead of potentials, has been proposed in the literature. In this work we elaborate and improve this proposal. We also use this formalism to confront the electric-magnetic duality symmetry of the electromagnetic field and the Aharonov–Bohm effect, two subtle aspects of electrodynamics that we examine in a novel way. We show how the former can be derived from the simple harmonic oscillator character of vacuum electrodynamics, while also demonstrating how the magnetic version of the latter naturally arises in an explicitly non-local manner. Full article
(This article belongs to the Special Issue Symmetry in Electromagnetism)
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Figure 1

Figure 1
<p>Experimental setup we will consider to analyse the magnetic AB effect. A source of electrons is located at the point <math display="inline"><semantics> <msub> <mi mathvariant="bold">x</mi> <mn>1</mn> </msub> </semantics></math>, from which one is emitted at a time <math display="inline"><semantics> <msub> <mi>t</mi> <mn>1</mn> </msub> </semantics></math>. Between the source and a screen on the other side of the setup there is a wall, containing two slits A and B, and a long impenetrable cylinder behind it. Inside the cylinder, oriented parallel to the z-axis, there is a magnetic field <math display="inline"><semantics> <mrow> <mi mathvariant="bold">B</mi> <mo>=</mo> <mover accent="true"> <mi mathvariant="bold">z</mi> <mo>^</mo> </mover> <msub> <mi>B</mi> <mn>0</mn> </msub> </mrow> </semantics></math>, while outside <math display="inline"><semantics> <mrow> <mi mathvariant="bold">B</mi> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>. The electrons can trace two types of <math display="inline"><semantics> <mi mathvariant="italic">deterministic</mi> </semantics></math> paths to reach the point <math display="inline"><semantics> <msub> <mi mathvariant="bold">x</mi> <mi mathvariant="normal">f</mi> </msub> </semantics></math> on the screen at a time <math display="inline"><semantics> <msub> <mi>t</mi> <mi mathvariant="normal">f</mi> </msub> </semantics></math>, either above (e.g., <math display="inline"><semantics> <msub> <mi>γ</mi> <mn>1</mn> </msub> </semantics></math>) or below (e.g., <math display="inline"><semantics> <msub> <mi>γ</mi> <mn>2</mn> </msub> </semantics></math>) the cylinder.</p>
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<p>Complex plane representation of <math display="inline"><semantics> <mrow> <msub> <mi>z</mi> <mn>0</mn> </msub> <mo>=</mo> <mi>x</mi> <mo>+</mo> <mi>i</mi> <mi>y</mi> </mrow> </semantics></math> outside and inside the cylinder.</p>
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12 pages, 247 KiB  
Article
Topologically Protected Duality on The Boundary of Maxwell-BF Theory
by Alberto Blasi and Nicola Maggiore
Symmetry 2019, 11(7), 921; https://doi.org/10.3390/sym11070921 - 15 Jul 2019
Cited by 5 | Viewed by 2617
Abstract
The Maxwell-BF theory with a single-sided planar boundary is considered in Euclidean four-dimensional spacetime. The presence of a boundary breaks the Ward identities, which describe the gauge symmetries of the theory, and, using standard methods of quantum field theory, the most general boundary [...] Read more.
The Maxwell-BF theory with a single-sided planar boundary is considered in Euclidean four-dimensional spacetime. The presence of a boundary breaks the Ward identities, which describe the gauge symmetries of the theory, and, using standard methods of quantum field theory, the most general boundary conditions and a nontrivial current algebra on the boundary are derived. The electromagnetic structure, which characterizes the boundary, is used to identify the three-dimensional degrees of freedom, which turn out to be formed by a scalar field and a vector field, related by a duality relation. The induced three-dimensional theory shows a strong–weak coupling duality, which separates different regimes described by different covariant actions. The role of the Maxwell term in the bulk action is discussed, together with the relevance of the topological nature of the bulk action for the boundary physics. Full article
(This article belongs to the Special Issue Duality Symmetry)
14 pages, 289 KiB  
Article
On the Electric-Magnetic Duality Symmetry: Quantum Anomaly, Optical Helicity, and Particle Creation
by Iván Agulló, Adrián Del Río and José Navarro-Salas
Symmetry 2018, 10(12), 763; https://doi.org/10.3390/sym10120763 - 17 Dec 2018
Cited by 11 | Viewed by 3003
Abstract
It is well known that not every symmetry of a classical field theory is also a symmetry of its quantum version. When this occurs, we speak of quantum anomalies. The existence of anomalies imply that some classical Noether charges are no longer conserved [...] Read more.
It is well known that not every symmetry of a classical field theory is also a symmetry of its quantum version. When this occurs, we speak of quantum anomalies. The existence of anomalies imply that some classical Noether charges are no longer conserved in the quantum theory. In this paper, we discuss a new example for quantum electromagnetic fields propagating in the presence of gravity. We argue that the symmetry under electric-magnetic duality rotations of the source-free Maxwell action is anomalous in curved spacetimes. The classical Noether charge associated with these transformations accounts for the net circular polarization or the optical helicity of the electromagnetic field. Therefore, our results describe the way the spacetime curvature changes the helicity of photons and opens the possibility of extracting information from strong gravitational fields through the observation of the polarization of photons. We also argue that the physical consequences of this anomaly can be understood in terms of the asymmetric quantum creation of photons by the gravitational field. Full article
(This article belongs to the Special Issue Symmetry in Electromagnetism)
30 pages, 1866 KiB  
Review
Symmetries, Conserved Properties, Tensor Representations, and Irreducible Forms in Molecular Quantum Electrodynamics
by David L. Andrews
Symmetry 2018, 10(7), 298; https://doi.org/10.3390/sym10070298 - 23 Jul 2018
Cited by 22 | Viewed by 5591
Abstract
In the wide realm of applications of quantum electrodynamics, a non-covariant formulation of theory is particularly well suited to describing the interactions of light with molecular matter. The robust framework upon which this formulation is built, fully accounting for the intrinsically quantum nature [...] Read more.
In the wide realm of applications of quantum electrodynamics, a non-covariant formulation of theory is particularly well suited to describing the interactions of light with molecular matter. The robust framework upon which this formulation is built, fully accounting for the intrinsically quantum nature of both light and the molecular states, enables powerful symmetry principles to be applied. With their origins in the fundamental transformation properties of the electromagnetic field, the application of these principles can readily resolve issues concerning the validity of mechanisms, as well as facilitate the identification of conditions for widely ranging forms of linear and nonlinear optics. Considerations of temporal, structural, and tensorial symmetry offer significant additional advantages in correctly registering chiral forms of interaction. More generally, the implementation of symmetry principles can considerably simplify analysis by reducing the number of independent quantities necessary to relate to experimental results to a minimum. In this account, a variety of such principles are drawn out with reference to applications, including recent advances. Connections are established with parity, duality, angular momentum, continuity equations, conservation laws, chirality, and spectroscopic selection rules. Particular attention is paid to the optical interactions of molecules as they are commonly studied, in fluids and randomly organised media. Full article
(This article belongs to the Special Issue New Trends in Quantum Electrodynamics)
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Figure 1

Figure 1
<p>Three topologically distinct time-ordered diagrams (time progressing upwards) for hyper-Raman scattering from an input mode <b><span class="html-italic">k</span></b> into an output mode <math display="inline"><semantics> <msup> <mi>k</mi> <mo>′</mo> </msup> </semantics></math>: the molecule undergoes a transition <math display="inline"><semantics> <mrow> <mi>n</mi> <mo>←</mo> <mi>m</mi> </mrow> </semantics></math> via two virtual intermediate states <span class="html-italic">r</span> and <span class="html-italic">s</span>.</p>
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<p>State-sequence diagram (time progressing to the right) for hyper-Raman scattering, subsuming all three pathways exhibited in <a href="#symmetry-10-00298-f001" class="html-fig">Figure 1</a>. Here, the interactions denoted by line sequences are colour-coded to highlight the input and output modes.</p>
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<p>Illustration of coupling weights <span class="html-italic">j</span><sub>1</sub> and <span class="html-italic">j</span><sub>2</sub>, in a partially inner, partially outer products of two tensors, of respective ranks <span class="html-italic">n</span><sub>1</sub> and <span class="html-italic">n</span><sub>2</sub>, as given by Equation (35). Assuming <span class="html-italic">j</span><sub>1</sub> &gt; <span class="html-italic">j</span><sub>2</sub>, the span of weights in the product may range from <span class="html-italic">j</span><sub>1</sub> − <span class="html-italic">j</span><sub>2</sub> to <span class="html-italic">j</span><sub>1</sub> + <span class="html-italic">j</span><sub>2</sub>, capped by an upper limit <span class="html-italic">n</span><sub>1</sub> + <span class="html-italic">n</span><sub>2</sub> − 2<span class="html-italic">p</span> that is the rank of the product tensor.</p>
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<p>Key time-ordered diagrams for engaging a static magnetic field <b><span class="html-italic">B</span></b> in the absorption of a single photon of wave-vector <b><span class="html-italic">k</span></b>. The diagram on the left represents the leading term, where the red circles denote E1, E2, or M1 coupling. Additional coupling with the static field (empty blue circle) engages two distinct time-orderings.</p>
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<p>State-sequence diagram for magnetic field engagement in single-photon absorption, connectors coloured to match the time-ordered representations of <a href="#symmetry-10-00298-f004" class="html-fig">Figure 4</a>.</p>
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<p>Cross-term for magnetic field engagement in single-photon absorption (Wagnière and Meier depiction). Such diagrams signify partial rate contributions, as compared with the individual matrix element depictions in <a href="#symmetry-10-00298-f004" class="html-fig">Figure 4</a> and <a href="#symmetry-10-00298-f005" class="html-fig">Figure 5</a>.</p>
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